3605
Inorg. Chem. 1994, 33, 3605-3608
n-Arene Complexes. 10.' Arene Distortions in
n-Arene Complexes of Chromium by Ring Substituents. Crystal Structure of (.rll:.rl6-C6HS{TiCpzCl~)Cr( C0)3
Table 1. Crystallographic Data for (?1:?6-C6Hs(TiCp2C1J)Cr(co)3 formula C19HlsO&ICrTi V,A3 1724.w) mol wt space group cryst syst a, A
Rita Meyer, Minet Schindehutte, Petrus H. van Rooyen, and Simon Lotz' Department of Chemistry, University of Pretoria, Pretoria 0002, South Africa Received November 24, 1993
Introduction The interaction of ring substituents of benzene and the resulting changes in charge distributions in the ring have been the topic of many studies in physical organic chemistry.2 While electronic disturbances in the u-bonds originate from inductive effects, resonance effects are observed in the n-system of the ring. Ring distortions in substituted benzenederivatives, incontrast to typical bond distances of 1.397(1) A and angles of 120° (sp2-hybridization) in benzene,3 are manifested in the lengthening or shortening of bonds and angular deformations especially around the ipsocarbon. Steric constraints caused by bulky substituents can also result in ring distortions! Benzene coordinated to chromium tricarbonyl in the $-fashion affords a planar ring with carbon atoms equidistant from the metal.5 Crystal structure determinations of a number of heterobimetallic complexes with u,n-arene bridging ligands have been recorded in our laboratories.6-7 Small but significant distortions in the arene ring occur mainly at the ipso-carbon atom bonded to the transition metal fragment. Recently Hunter and co-workers8 discussed ring distortions of analogous complexes solely on the basis of n-interaction between the transition metal substituent and the 7-system of the arene ring. Significant n-donation from FeCp(C0)z substituents in bi- and trimetallic n-arene complexes of chromium was recorded. We have observed similar ring distortions in the structural data for the bimetallic complexes (s1:r16-o-C6H4R(TiCp2CI))CT(C0)3 (R = H ( l ) , F6 (2), OMe9 (3)). Little evidence of multiplebonding interactions between the ipso-carbon and the u-bonded transition metal was observed in the titaniumsarbon bond distances of 1-3. Furthermore, titanium is formally in a +4 oxidation state in these complexes, which implies empty d orbitals and rules out any n-donation from the metal. Therefore, to obtain a more complete picture of arene distortions in u,n-coordinated bimetallic complexes, we wish to discuss distortions on the premise ( 1 ) Part 9: Van Rooyen, P. H.; Schindehutte, M.; Lotz, S. Inorg. Chim.
Acta 1993, 208, 207. (2) See, for example: (a) Maskill, H. The Physical Basis of Organic Chemisrrv: Oxford University Press: New York, 1985. (b) Katritzky, A. R.; Tdpsom, R. D. Angew. Chem., Int. Ed. Engl. 1970, 9,87. (3) (a) Ermer, 0. Angew. Chem., Int. Ed. Engl. 1987, 26, 782. (b) X-ray diffraction of benzene at 270 K Cox, E. G.;Cruickshank, D. W. J.; Smith, J. A. S. Proc. R. SOC.London 1958, A247, 1. (c) Neutron diffraction of benzene at 138 and 218 K Bacon, G.E.; Curry, N. A.; Wilson, S. A. Proc. R. SOC.London 1964, A279, 98. (d) Gas electron diffraction: Tamagawa, K.; Iijima,T.; Kimura, M.J . Mol. Struct. 1976, 30, 243. (4) Bock, H.; Ruppert, K.; Nither, C.; Havlas, 2.; Herrmann, H.-F.; Arad, C.; GBbel, I.; John, A.; Meuret, J.; Nick, S.; Rauschenbach, A.; Seitz, W.; Vaupel, K.;Solouki, B.Angew. Chem.,Int. Ed. Engl. 1992,31,550. ( 5 ) Muetterties, E. L.;Bleeke, J. R.; Wucherer,E. J.; Albright,T. A. Chem. Rev. 1982, 82, 499. (6) Van Rooyen, P. H.; Schindehutte, M.; Lotz, S. Organometallics 1992, 11, 1104. (7) Lotz, S.;Schindehutte, M.; Van Rooyen, P. H. Organometallics 1992, 1 1 , 629. (8) Hunter, A. D.; McDonald, R.; Santariero, B. D.; Bott, S. G.; Atwood, J. L. Organometallics 1992, 11, 3050. (9) Meyer, R.; Lotz, S.; Van Rooyen, P. H. Unpublished results.
0020-1 6691941 1333-3605$04.50/0
6,A
c, A I%
z
deg
"R
426.65 P 2 l / n (No. 14) monoclinic 10.493(2) 12.249(2) 13.975(2) 106.21(1) 4
Z(IFo1
- IF&/ZlFol.
bRw
&Ic, g cm4 p(Mo Kru), cm-I F(OO0) no. of data measd no. of data used ( D o , ) no. of parms refined
R" RWb
1.64 11.82 864 2739 2616 227 0.049 0.034
[Zw(lFd - lFc1)2/Z~Fo12]1/2; w =
Up,-?
that they could also originate from inductive charge effects in the a-frame of the arene ring. We have also investigated the effect of organic substituents with different electronegativities, ortho to the titanium moiety, on the magnitude of theangular deviation around the ipso-carbon atom bonded to titanium.
Experimental Section The reaction and subsequent manipulations were performed by using conventional techniques for the handling of air-sensitive compounds.1° Solvents were purified, degassed, and dried according to standard procedures.I1 The column packing for liquid column chromatography consisted of Si02 (0.0634.200 mm), and the separation was performed on a column cooled by recycling cold methanol (-20 "C) through the column jacket. Prior to use, dichloromethane was distilled from P 2 0 5 ; hexane and benzene were distilled from sodium wire, while tetrahydrofuran was freshly distilled from sodium-benzophenone ketyl under inert atmosphere. The chromium precursor ( ? J ~ - C ~ H ~ ) C ~was ( C Oprepared )~ according to the published procedure12 and was lithiated according to the method described by Card and Trahanov~ky.~'The bimetallic complex (~jl:$-CaHs(TiCp2Cl))Cr(CO)3 (1) was synthesized by modifying a procedure reported earlie@ and checked against an authentic sample. Synthesis. heparation of ( ~ L : ~ 6 - C 6 H ~ ~ T i C p 2 c ~ } ) A c rcooled (co)~. solution (-70 "C) of 0.64 g (3 mmol) of (76-benzene)tricarbonylchromium(0) in 30 mL of T H F was treated dropwise with 2.1 mL of a 1.6 mol/dm' solution of butyllithium (3.3 mmol). The mixture was stirred for 20 min while the temperature was raised to -30 OC. This freshly prepared (Tj64ithiobemene)tricarbonylchromium(O) solution was cooled to -50 "C and added to an equimolar solution of CpzTiClz (0.78 g, 3 mmol) in T H F (30 mL) at -78 OC. After being stirred for 30 min, the reaction mixture was allowed to warm to room temperature and stirring was continued for 1 h. Removal of the solvent under reduced pressure gave a black-green solid, which was subjected to column chromatography onsilica gel. Elution with a dichloromethane-hexane mixture (1:l) yielded a yellow fraction, which was identified as the unreacted chromium starting material, followed by a blue-green zone containing (?+:~j~-C&(TiCp2CI))Cr(CO), (1). In addition, a number of other bands observed in low yield were not collected and identified. After removal of the solvent, the residue was dissolved in a minimum of dichloromethane, and the solution was filtered through a plug of Celite, after which an equal volume of hexane was carefully layered on top of the filtrate. The Schlenk tube was left undisturbed at -4 OC for several days, after which the mother liquor was decanted and the remaining crystals were dried in vacuo. Yield: 0.44 g (69%). X-ray Crystallographic Analysis. Crystallographic data for (w1:q6C6Hs(TiCp2C1))Cr(Co),, measured a t 294 K, are listed in Table 1. Accurate unit cell parameters were obtained by least-squares methods from the positions of 25 carefully selected centered reflections (15' < B < 18O), using a black crystal with approximate dimensions 0.15 X 0.16 X 0.17 mm3. By application of 0-28 scan techniques and the use of monochromat4 Mo Ka radiation (A = 0.7107 A) on an Enraf-Nonius CAD4 diffractometer with an aperture of 1.3 X 4.0 mm3, the intensity data for h = 0, +13, k = -15,0, and I = -17, +17 were collected in the (10) Perrin, D.; Armarego, W. L.; Perrin, D. R. Purification of Loboratory Chemicals, 2nd ed.; Pergamon: New York, 1980. ( 1 1 ) Shriver, D. F.; Drezdon, M. A. The Manipulation of Air-Sensitive Compounds, 2nd ed.; John Wiley and Sons: New York, 1986. (12) Mahaffy, C. A.; Pauson, P. L. Inorg. Synrh. 1979, 19, 154. (13) (a) Card, R. J.; Trahanovsky, W. S. J . Org. Chem. 1980,45,2555. (b) Card, R. J.; Trahanovsky, W . S.J. Org. Chem. 1980,45, 2560.
0 1994 American Chemical Society
3606 Inorganic Chemistry, Vol. 33, No. 16, 1994
Notes Table 2. Fractional Atomic Coordinates (Xlw) and Equivalent Thermal Factors (X l @ A') for (n*:n6-CaHalTiClhC1~)Cr(CO)a ~~
atom Cr c1 01 c2 02 c3 03 c4 c5 C6 c7
cs
Figure 1. Perspective drawing of the molecular structure of 1.
c9 Ti c10 c11 c12 C13 C14 C15 C16 C17 C18 C19
c1
xla ~~
vlb
zlc
u-4
1460(1) 729(4) 254(3) 2498(4) 3 125(3) 647(4) 148(3) 2657(4) 27 12(5 ) 1780(5) 765(5) 711(4) 1664(4) 1524(1) 1760(5) 2697(5) 3145(4) 2467(4) 879(5) 1576(4) 1885(4) 2683(4) 2185(5) lOSS(5) -350( 1)
2168(1) i07ii3j 402(2) 1354(3) 859(3) 1985(3) 186l(3) 2881(3) 3362(4) 3773(3) 3673(3) 31 98(3) 2799(3) 2371(1) 818(3) 1328(3) 1442(3) 975(3) 3676(4) 586(3) 3350(3) 3585(3) 4041(3) 4 101(3) 2029( 1)
30( 1
~
-3347( 1) -3 107(5) -2992(4) 4395(5) -5084(4) 4858(5) -5817(4) -1738(5) -2747(5) -3 147(5) -2557( 5 ) -1 554(4) -1 08 1(4) 8 W ) 1300(5) 1635(5 ) 468(5) -580(5) 2652(5) -79(5) 30 12(5) 2211(5) 1363(5) 162l(5) 589( 1)
Table 3. Selected Bond Distances
x
U
LJ Figure 2. View of 1 along the Cr-arene bond. range 3 I 0 5 27O. There was no significant crystal decay, as indicated by monitoring the intensities of three standard reflections throughout the data collections. The data werecorrected for absorption (empirical, based on the azimuthal scans for nine reflections of the crystal), as well as for Lorentz-polarization effccts. The maximum, minimum, and average transmission factors were 1.OOO,0.980.and0.993, respectively. Equivalent reflections were merged (Rht = 0.020). The structure was solved by conventional Patterson and Fourier techniques using SHELX86.14 All the non-hydrogen atoms were refined anisotropically,'s and the hydrogen atoms were placed in calculated positions and refined with a common isotropic thermal parameter that converged to Vi,= 0.060(4) AZ. Perspective drawings of the molecule shown in Figure 1, illustrating the crystallographic numbering scheme used, and Figure 2, a projection on the benzene plane displaying the relative conformation of the (arene)Cr(CO), moiety, were prepared with ORTEP.16 Atomic scattering factors were taken from the l i t c r a t u r ~ . ~ ~ There were no corrections for the presence of extinctions made. Final atomic coordinates and equivalent isotropic thermal parameters and selected bond lengths and angles appear in Tables 2 and 3, respectively.
Results and Discussion The general features of the molecular structure of (VI:$C6H&TiCpzClJ)Cr(CO)3(1) are consistent with those recorded for (tlL:~6-CgH~R~TiCp2C1))cr(co)3 (R = 0-F, pMe).6 The Cr-C(arene) distances of 1 are identical within experimental error (Cr-C(arene) = 2.239(5) A averaged), and the CrPh(center)-C9 and Cr-Ph(center)-C6 angles of 92.2 and 89.2O, (14) Sheldrick, G. M. SHELX 86: A program for the solution of crystal structures. University of G(lttingen, 1986. (15) Sheldrick, G.M. SHELX 76: Program for Crystal Structure Determination; University of Cambridge, 1976. (16) Johnson, C. K. ORTEP. Report ORNL-3794; Oak Ridge National Laboratory: Oak Ridge, TN, 1965. (17) (a) International Tables for X-ray Crystallography; Kynoch Press, Birmingham, U.K.,1974; Vol. IV.(b) Cromer, D. T.; Liberman, D. J. Chem. Phys. 1970,53, 1891.
(A) and Angles (deg) for 1
Cr-C 1 Cr-CZ Cr43 Cr-C(arene) c1-01 c2-02 c3-03 Ti49 Ti41
Bond Distances 1.852(2) Ti-C(cpA) Ti-C(cpB) 1.850(5) 1.829(5) c944 2.239(5)O c4-a 1.137(5) (2x6 1.146(5) c647 1.148(5) C7-C8 2.228(4) C849 2.343(1)
2.376(5)' 2.39O( 5)e 1.41 8(6) 1.405(6) 1.394(7) 1.41 3(7) 1.395(6) 1.439(6)
C14r42 C2-Cr43 C3-Cr-Cl Cr-Cl-01 Cr42-02 c443-03 Ti-C9-C4
Bond Angles 91.0(2) C8-C9-C4 86.9(2) c9-Ce5 86.2(2) C4-C5-C6 C5-CM7 177.5(5 ) CM7-CS 177.4(5 ) 179.0(4) C7-C8-C9 125.1(3)
115.9(4) 121.9(5) 120.8(5) 119.3(5) 119.9(5) 122.2(5)
The averaged value.
respectively, indicate that the Cr-Ph vector is almost normal to the approximate plane of the arene ring. The planar benzene ring indicates that the Cr(CO)s moiety is bonded to the *-cloud of the bridging arene ligand which is also u-bonded to the TiCpzC1 unit. The titanium is in a distorted tetrahedral environment of ligands. The Ti-C9 distance of 2.228(4) A does not differ significantly from the reported distances of 2.21 A for the Ti-C(sp3, methyl) bond in (s*-C9H7)2Ti(CH3)2,L8the 2.216 A distance for the TiC(sp2, phenyl) bond in ( $ - C ~ ) Z T ~ ( ~ C ~ H ~ Cand H ~the )Z,~~ corresponding distances of 2.217(8) and 2.213(6) A for (t+:$C6H,R(TiCpzCl))Cr(CO)p where R = o-F (2) and p-CH3P respectively. In contrast, Ti-C distances with perceivable *-interaction contributions between the titanium and a carbon atom are significantly shorter and fall in the range 2.00-2.10 A.m Therefore, the Ti-C(arene) bond lengths in the bimetallic (18) Attwood, J. L.; Hunter, W.E.;Hrncir, D. C.; Sameul, E.;Alt, H. Inorg. Chem. 1975,14, 1757. (19) Zeinstra. J. D.; Teuben, J. H.; Jellinek, F.J. Orgammer. Chem. 1919, 170, 39.
Notes
Inorganic Chemistry, Vol. 33, No. 16, 1994 3607
Table 4. Orientation of the Carbonyl Ligands with Respect to the TiCp2C1 Substituent (deg) angle' 1 26 3c 91 98.6 92.2 67.8,41.5 188.3, 159.8 92 216.9 211.7 $3 334.5 327.6 308.1,280.6 0 9" measured in a clockwise direction from the Ti substituent to the nth carbonyl. b Reference 6. Two Nonequivalent molecules in the unit cell. Reference 9.
TiCp2CI
I
Figure 3. Labels used for bond distances and angles of 1-3.
compounds (1-3) suggest little, if any, multiple bonding interaction between the titanium and the arene carbon atom. A view from above the arene plane is shown in Figure 2. The Cr(C0)3 fragment lies in a nearly staggered conformation, experiencing a 25.5' anticlockwise rotation from the fully syneclipsed conformation and a 34.5' clockwise rotation from the alternate anti-eclipsed structure. A syn-eclipsed geometry is the preferred structure for monosubstituted (~f-arene)Cr(CO)~ molecules with electron-donating functional groups, and an antieclipsed conformation is favored for electron-withdrawing groups.5 In Table 4 carbonyl orientations with respect to the titanium substituent are compared. Conformational analysis of Cr(CO)3 tripod orientations for 1-3 suggests that the titanium fragment can best be described as a electron-donating substituent. Spectroscopic and structural data6 of 1-3 indicate a polarized TiC(arene) a-bond in which the electron density is shifted toward the arene ring. Deviations from a fully syn-eclipsed orientation in 1 are ascribed to steric factors. Small deviations from ideal benzene bond distances and angles3 are observed around the ipso-carbon atom of 1. The endocyclic bondangle,cu,isreducedto115.9O (Aa=-4.l0)andtheadjacent bonds, a and a', are lengthened by 0.025 A (1.429(6) A averaged) compared with the remaining four distances (1.404(7) A, average of b, b', c, and c'; see Figure 3). The adjacent angles, j3 and j3' (1 2 1.9 and 122.2O), are on average increased by -Acyl2 to reduce the ring strain caused by these distortions. Coulson and coworkers2' reported a linear dependency of the endocyclic bond angles on the Pauling's electronegativity values of substituents in monosubstituted benzene derivatives. They also suggested that the deviation for the j3 angles was close to - P a l 2 and that the deviation of the y angles was approximately 0'. A method developed by Norrestam and Schlepper22for estimating deviations in substituted benzene derivatives was based on a set of deformation parameters and confirmed conclusions made by Coulson and co-workers. The fact that a similar correlation was found for 1 suggests that the deformation of the arene ring is dependant not on the r-coordination of the arene ring to the Cr(CO)3 fragment but solely on inductive electronic and steric properties of the a-coordinated substituent. (20) (a) Binger, P.; Miiller, P.; Phillips, P.;Gabor, P.; Mynott, R.; Herrmann, A. T.; Langhauser, F.; Kriiger, C. Chem. Ber. 1992, 125, 2209. (b) Francl, M. M.; Hehre, W. J. Organometallics 1983,2,457. (c)Beckhaus, R.; Flatau, S.; Trojanov, S.; Hofmann, P. Chem. Ber. 1992, 125, 291. (d) Rappe, A. K. Organometallics 1987, 6, 354. (21) Domenicano, A.; Vaciago, A.; Coulson, C. A. Acto Crystollogr. 1975, 831, 1630. (22) Norrestam, R.; Schlepper, L. Acto Chem. S c a d . 1981, ,435, 91.
Table 5. Arene Distortions' of (111:116-C6H~R(TiCp2CI))Cr(CO)) (R = 1 ( 0 , F (21, OMe (3))
1 U
a'
b b'
2
36
Bond Lengths (A) 1.418( 6) 1.396( 11) 1.439(6) 1.431(11) 1.405(6) 1.393(12)
1.404(8)
1.395(6)
1.400(8)
c
1.394(7)
C'
1.413(7)
1.390(12) 1.381( 12) 1.395( 12)
1.401(8) 1.443(8)
1.387(9) 1.387(9)
Bond Angles (deg) 115.9(4) 11 1.3(7) 113.4(6) B 121.9(5) 126.3(9) 124.2(6) B' 122.2(5) 122.9(9) 123.5(6) 7 120.8(5) 120.7(9) 119.5(7) 7' 119.9(5) 122.8(9) 119.3(7) 6 119.3 ( 5 ) 115.7(9) 120.1(7) Distances from Plane (A) and Angles between Planes (deg) plane defined C 4 4 5 - C d C 7 C5-C6-C7-C8 C5-C6-C7-C8 6, 6Ti 0.509(7) 0.546(2) 0.405(12) 6c9 0.038(8) 0.069(8) 0.040(14) 6R 0.129(6) 0.216(14) 0.063( 14) 0.039(10) 2.7(4) 3.7(8) 2.0(5) Dihedral Angle (deg) CB-Cg-Ti-CI 27.4(3) 22.5(6) 21.8(4) Numbering of bond distances and angles according to Figure 3. bAverage value of two nonequivalent molecules in the unit cell. Magnitude of the displacement of the atom from the defined plane. Angle between the C449-C8 plane and the defined plane. a
2
The Hunter model8 predicted the direction of deviation in substituted ?r-arene complexes of chromium on the basis of the resonance effects of known organic ?r-donor and r-acceptor substituents. In contrast, an approach based on the inductive effects of the more electropositive titanium substituent in the bimetallic complexes 1-3 can be applied satisfactorily to account for observed distortions. Furthermore, it has become an accepted practiceinorganicchemistry to treat a- and r-effectsof substituted benzene derivatives independently.zbJ3 The electropositive Ti substituent will interact with a sp2-hybrid orbital of the phenyl ring with relatively mores and less p character to form the Ti-C(arene) a-bond. As a result, the remaining two sp2-hybrid orbitals of the ipso-carbon, which form the a-frame of the ring, will have more p and less s character. Therefore, the endocyclic angle will decrease, causing the a and a' bonds to lengthen. To relieve the resulting ring strain in the a-system of the benzene ring, the arene ligand will distort in such a way that steric interactions are minimized. Thus, the ipso-carbon and titanium substituent will move away from the Cr(CO)3 moiety towards the open side of the arene ring. These arguments are consistent with the structural data for 1, where a displacement of 2.7(4)O out of the plane of the arene ring and away from the chromium tricarbonyl is recorded, and with literature refere n c e ~describing ~ ~ ~ ~ phenyl , ~ ~ distortions in organic molecules. The deviations from ideal benzene values are small compared to distortions of 35-45' for ipso-carbons of sp3-hybridization in cyclohexadienyl c o m p l e ~ e s . ~ ~ ~ ~ ~ The magnitude of the distortion is expected to correlate with the electronegativity of the substituent attached to the benzene ring. To test this assumption, we investigated the effect of an additional substituent of different electronegativity in the position ortho to the Cp2TiC1substituent. Arene distortion data for the bimetallic complexes (ql :s6-o-C6H4R(TiCp2C1J)Cr(CO)s (R = H, OMe, F) are summarized in Table 5 . The substituents, OMe (23) Allen, H. A.; Kennard, 0.;Taylor, R. Acc. Chem. Res. 1983, 16, 146. (24) Maezke, T.; Seebach, D. Helu. Chim. Acto 1989, 72, 624. (25) Niemer, B.; Steimann, M.; Beck W.Chem. Ber. 1988, 121, 1767. (26) Semmelhack, M.F.; Hall, H. T., Jr.; Farina, R.; Yoshifuji, M.; Clark, G.; Bargar, T.; Hirotsu, K.; Clardy, J. J. Am. Chem. SOC.1979, 101, 3535.
3608 Inorganic Chemistry, Vol. 33, No. 16, 1994
Notes
Internal angles 130 1
I
t
lZO
substituent are shown in Figure 4. Although only three data points are available and their differences are small relative to the standard deviations, a definite pattern emerges. Linear correlations exist between the internal bond angles (aor 8) and Pauling’s electronegativitiesof the heteroatoms of the substituents ortho tothetitaniumfragment. Thedependencyofaonxdemonstrates the cooperativeeffect of the substituents in enhancing distortions of the planar arene ligand.
Coaclusion
105
I
2
2.2
2.4
2.6
2.8 3 3.2 3.4 3.6 Pauling electronegativity
3.8
4
4.2
Figure 4. Endocyclic angles (a,8) versus Pauling electronegativities ( x ) . A vertical bar shows the error range ( H u )of each p i n t .
and F, should, because of their electron-withdrawingproperties, assist in increasing the p and decreasing the u angles. Owing to the relative positions of the substituents on the arene ring, the two effects are synergic and the magnitude of the distortions will depend directly on the electronegativity of the R substituent. While the decrease in the a angle results in substantial increases in the p and p’ angles, the increases in the fl angles do not affect the adjacent y and y’ angles significantly. Plots of the internal angles u and Buersus Pauling’s electronegativity ( x ) oftheorganic
This study has shown that r-coordination to the Cr(CO)3 fragment does not significantlyaffect the geometry of the planar arene ring and that distortions of the ring, irrespective of substituents being organic or transition metal fragments, are determined by the inductivepropertiesofthe u-bondedsubstituent. Thus, models based on resonance8 and inductive effects of substituents can be used to explain structural deviations of substituted benzene derivatives when they are present as ligands in organometallic chemistry.
Acknowledgment. This research was supported in part by the Foundation for Research and Development (FRD), Pretoria. lWterhiAnihML: Tables of bond distanca and angles, anisotropic temperature factors, and hydrogen atom coordinates, as well asan ORTEP plot of the unit cellcontents (5 pages). Ordering information is given on any current masthead page.
